F1 = F2 · e^(μ·θ)
Calculate tight-side tension, slack-side tension, friction coefficient or wrap angle with the capstan (Euler–Eytelwein) equation. The belt tension ratio F1/F2 grows exponentially with belt friction and wrap angle.
Calculate tight-side tension, slack-side tension, friction coefficient or wrap angle with the capstan (Euler–Eytelwein) equation. The belt tension ratio F1/F2 grows exponentially with belt friction and wrap angle.
Select a target and calculate.
According to the capstan (Euler–Eytelwein) equation, F₁ grows exponentially with μ·θ: every additional bit of wrap multiplies the transmissible force. At θ = 0, F₁ = F₂ (dashed). The marker shows the entered wrap angle.

Calculate tight-side tension, slack-side tension, friction coefficient or wrap angle with the capstan (Euler–Eytelwein) equation. The belt tension ratio F1/F2 grows exponentially with belt friction and wrap angle.
μ = 0.3 and θ = 180° (π rad) give a maximum tight-side tension of about 256.7 N at F2 = 100 N.
At the point of impending slip; centrifugal effects and belt stiffness are excluded.
This calculator solves the capstan equation – also known as the Euler–Eytelwein equation or belt friction equation – for the missing quantity among tight-side tension F1, slack-side tension F2, friction coefficient μ and wrap angle θ. It answers the central question of belt drive design: how large can the belt tension ratio F1/F2 become before the belt slips on the pulley?
At the point of impending slip, the belt tension ratio between the tight side and the slack side depends exponentially on belt friction and wrap angle: F1/F2 = e^(μθ), with θ in radians. Roloff/Matek writes this as m = F1/F2 = e^(μβ̂) and calls m the strand-force ratio; the ratio is always evaluated with the wrap angle of the small pulley, where slip starts first. The same relationship – historically Euler's, later Eytelwein's – applies to any rope, band or belt sliding over a cylinder, which is why it is also called the capstan equation.
A sailor can hold a heavily loaded line with little hand force by wrapping it several times around a capstan or cleat: every extra turn adds 2π to the wrap angle θ and multiplies the holdable tension difference. A belt drive uses exactly this belt friction effect – the pulley is the capstan, the tight side carries the load and the slack side is the hand.
F1 = F2 · e^(μ·θ)
F1 = F2 · e^(μθ)F2 = F1 · e^(−μθ)μ = ln(F1/F2) / θθ = ln(F1/F2) / μ| Symbol / input | Meaning |
|---|---|
| Tight-side tension F1 | The maximum tight-side tension at which the belt is on the verge of slipping on the pulley (the limiting case of the capstan equation). As a result it follows from F2·e^(μθ). |
| Slack-side tension F2 | The slack-side tension – the force in the loose belt strand, produced by the drive's pretension (e.g. a tensioning pulley or adjustable centre distance). |
| Friction coefficient μ | The sliding friction coefficient between belt and pulley surface. Source: the belt manufacturer's datasheet; typical value for a flat belt on metal is about 0.3, effectively higher for V-belts due to the wedging action. |
| Wrap angle θ | The wrap angle – the angle over which the belt contacts the pulley considered. Source: computed from the pulley diameters and center distance (see the wrap-angle calculator), or read from a drawing. |
Enter two of the four quantities. Use for θ the wrap angle at the pulley where slipping would occur first – normally the smaller pulley of an open belt drive. Use for μ the friction coefficient between the belt and the pulley surface; for V-belts and ribbed belts the effective wedge friction μ′ = μ / sin(α/2) with the groove angle α applies instead of the flat-belt value.
Select the target quantity and enter the other known values with units. The result describes the limiting case at the point of impending slip; for safe operation, the actual tension difference should keep a margin below this limit. To move from the tension ratio to the drive, take the effective tension Fₜ = F₁ − F₂ and, with belt speed, the transmitted belt power.
Given F2 = 100 N, μ = 0.3 and θ = 180° (π radians), substitution gives F1 = 100 · e^(0.3·π) ≈ 256.6 N, i.e. a belt tension ratio of about 2.57.
A maximum tight-side tension of 256.6 N at 100 N slack-side tension means that at most a tension difference of about 156.6 N can be transmitted under these conditions before the belt slips. This difference is the usable circumferential force; multiplied by the pulley radius it gives the maximum transmittable torque, and multiplied by belt speed the transmittable power. Roloff/Matek expresses the same result as the pull-out ratio κ = (m − 1)/m ≈ 0.61: only 61 % of the tight-side tension is available as effective tension.
Forces in newtons (N); the friction coefficient μ is dimensionless; the wrap angle may be entered in degrees or radians – the exponent itself always requires radians (θ[rad] = θ[°]·π/180).
The capstan equation underlies the design of flat, V- and ribbed belt drives, conveyor drives, winches and capstans, band brakes and rope clamps. In belt design it fixes, together with the wrap angle, how much effective tension a given pretension can deliver – see the drive-element calculators for the related belt and chain tools.
The equation describes the static limit immediately before slip for a massless, inextensible belt, and assumes that the whole wrap arc takes part in transmitting force. In real operation only the active arc transmits the circumferential force while the belt does not slide on the rest arc (Grashof), so the full wrap angle is a design assumption rather than a measurement. At higher belt speeds the centrifugal tension Fz = A·ρ·v² reduces the contact pressure; the capstan equation then has to be applied to the strand forces reduced by Fz, i.e. (F1 − Fz)/(F2 − Fz) = e^(μθ).
Common mistake: Do not substitute the wrap angle in degrees into the exponent – the calculator converts automatically, but a manual calculation must use radians. Do not use the flat-belt friction coefficient for a V-belt, and do not equate μ with the static friction of a dry, clean surface if the belt is worn, dusty or oily.
None in substance. Capstan equation is the common English name for the exponential belt friction law F1/F2 = e^(μθ); German machine-element literature attributes it to Eytelwein (Eytelweinsche Beziehung) and often also to Euler.
The smaller of the two wrap angles, usually at the small pulley, because the belt slips there first. The wrap angle calculator gives it from the pulley diameters and centre distance.
Take the difference between tight-side and slack-side tension (F1 − F2) as the effective tension, multiply it by the pulley radius for torque or by belt speed for power.
Because centrifugal force lifts the belt off the pulley and lowers the contact pressure. Only the strand forces reduced by the centrifugal tension Fz obey the capstan equation, so less effective tension remains for the same pretension.